Radio compass



Plasma sept. 21, 194s prior art.

Aircraft radio direction inders in present-day l commercial use employ a conventional loop antenna to determine direction and a non-directional antenna to resolve the 180 ambiguityof the figure-eight directivity pattern of the loop. The limitations of these direction finders have long been recognized. Some attemptsv have been made to overcome these limitations by installing conventional Adcock antenna' systems on aircraft, but, except at `very high frequencies, these attempts have been unsuccessful. It is now generally recognized that for low to mediumfrequency use the conventional .differentiallyconnected spaced-collector directional antenna systems cannot readily be applied to aircraft direction iinders.

It is therefore one of the objects oi this invention to provide a spaced-collector direction finder wherein the mode of operation does not require any directive properties in the antenna system.

It is another object of the invention to provide a spaced-aerial direction finder which is capable d of use on a small craft or the like. 6A"Erh' sin (@H'r su? a) (2) For a better understanding of the invention, y d

together with other and further objects thereof, 40 L reference is had to the following description tak- 6B Emh sm ne A Sm m (a) en in connection with the single figure of the accompanying drawing, which shows a block diagram of the invention.

In the drawing, there are shown two spaced non-directional antennas A and B which abstract from the received wave two signals differing in amended April 30, 1928; 370 0. G. T57) phase as a function of the direction of wave arrival. The two signals abstracted by antennas A and B are then amplitude-modulated independently by modulators it and It driven in opposite phase, at a low frequency rate, preferably, but not necessarily, in a sinusoidal fashion by the push-pull output of an audio oscillator 26. The

two amplitude-modulated signals thus obtained are then combined to produce a phase-modulated resultant signal. VThe amplitude of this phasemodulated resultant signal is substantially independent of the direction of arrival so long as the physical spacing between the antennas 'is small compared to the Wavelength of the received signal under consideration.

The phase-modulated resultant signal is then applied to a receiver i5 wherein it is detected, preferably as an equivalent frequency-modulated signal, to obtain a low frequency signal whose amplitude and sense are dependent upon the direction of arrival. This low frequency signal is then applied to an indicator, which may comprise a conventional synchronous detector and left-right meter, to produce directional indicat ons.

The operation of this direction finder will now be described in greater detail. Assume that antennas A and B are mounted on the right and left wings, respectively, of an aircraft. The radio frequency field (E) existing at a point which is midway between antennas A and B, may be denoted by the equation:

E= E,a sin wc! (l) where Em is the maximum amplitude and we is the angular frequency of the received signal. v The signal voltages eA and es induced in antennas A and B, respectively, may then be represented by the equations:

where The signals en and es are applied to modulators I3 and i6, respectively. The modulator outputs are then combined and applied to the input of receiver I5. The resultant signal at the receiver input is, therefore. the vector combination of the two amplitude modulated component signals ex and e'n represented by the following equations:

e'A=lt(1+a sin wut) sin (wet-+1? sin a) (4) v eB=k(1-a sin wut) sin (act-Ig sin a) (5) where:

k=a constant,

a=the amplitude-modulation factor, and

m=angular frequency of the low-frequency modulating oscillator Il.

" After expansion Equations 4 and 5 may be simplified by employing the following approximations:

is always small in any practical case.

The resultant signal at the input of receiver IB may therefore be represented adequately by approximate equations of the form:

egg2k(sin wot-i--d sin a sin mi cos mi) (8) The approximate Equation 9 neglects the small amount of amplitude modulation present in the resultant signal.` It is apparent from Equation 9 that this resultant signal is phase modulated at the modulating frequency of oscillator 2l to an extent determined by the direction of wave arrival.

The resultant signal, en, is passed through a superheterodyne receiver i5 which includes an R-F amplier i8. mixer i7, local oscillator i8, intermediate-frequency amplifier i9, and a monitoring channel comprising a detector 20, which may be designed to demodulate either amplitude modulated or frequency modulated waves, an audio amplifier 2|. and headphones 22.

Part of the signal output of I-F amplifier i9 is demodulated to produce a signal of the modulating frequency from which directional information can be obtained. Now, since this signal is phase modulated, it could be demodulated in a phase modulation detector. However, as is well known, phase modulation detectors are rather unstable and critical to adjust. It is preferable therefore to detect the phase modulated signal as an equivalent frequency-modulated signal.

Accordingly, this signal is passed through a limiter 25 to remove any amplitude modulation which may be present, then passed through a frequency-deviation expander 26 t'o produce a vsatisfactorily-high degree of frequency modulation. and finally is detected in a conventional frequency modulationvdetector 21. The output of the frequency modulation detector 21 is applied vthrough a synchronous rectifier I to a conventional left-right meter 3 i.

Part of the output from the oscillator 2l is applied to the synchronous rectifier ill through a 90 phase shifter 2l. The phase shifter is provided tov compensate for the 90 phase shift of the modulation which exists when a phase modulated signal is detected as an equivalent frequency modulated signal. The amplitude and sense of the detector output 'signal are compared with the output of oscillator 28 in synchronous rectifier lli and indicated in meter 3 I.

The functional elements shown only as blocks may take any one of the well-known conventional forms. The frequency-deviation .expander 26 may be oi' the type used in the well-known Armstrong frequency modulation system, wherein the phase-modulated signal is frequency-multiplied, and then heterodyned down to a lower mean irequency. This process may be repeated several times until a signal having the desired mean frequency and degree of frequency deviation is obtained.-

It will be apparent from the foregoing that I have provided a novel radio direction iinder employing spaced collector elements which need not sultant phase modulated signal is translated into directional information.

This method can of course be employed in direction finders of a much more elaborate form than the simple left-right radio compass illustrated in the drawing. For example, direct reading direction finders can be designed which employ four or more spaced collectors associated in pairs. Crossed-pointer presentation of directional information or any one of several wellknown forms of cathode-ray tube presentation can then .be used.

While there has been described what is at present considered a preferred embodiment of my invention, it will be obvious to those skilled in the art that various changes and modifications may be made therein without departing from the invention, and it is aimed in the appended claim to cover all such changes and modifications as fall within the true spirit and scope of the invention.

Iclaim:

A radio system comprising a plurality of spaced, non-directional aerials. a low-frequency sinewave oscillator for independently modulating in opposite phase the respective outputs of said aerials, means for combining the modulated waves to derive a resultant phase-modulated wave, a signal-monitoring channel and a compass channel excited in parallel by said resultant wave, said compass channel comprising means for limiting the amplitude and expanding the degree of phase modulation of said resultant wave, a frequency-modulation detector connected to the output of said Vlast named means for deriving a sine wave having a frequency equal to that of the output of said oscillator and a phase.

nous

BEFEBENGES CITED The following references are of record in the le of this patent:

Number UNITED STATES PATENTS Name Date Chiriex Feb. 6, 1934 Nickel Jan. 30; 1940 Wagstaie Sept. 3, 1940 Goldstein Dec. 22, 1942 vLoughren July 9, 1946v Goldstein Aug. 6, 1946 

